Second-order electrogyration effect in BSO crystal

被引:0
|
作者
Guerrero-V, Maria Alejandra [1 ,2 ,3 ]
Rueda-P, Jorge-Enrique [2 ]
机构
[1] Univ Pamplona, Fac Ciencias Bas, Dept Fis, Grp Opt Moderna MINCIENCIAS, Campus Principal, Pamplona 543050, Norte De Santan, Colombia
[2] CONICET CIC UNLP, Ctr Invest Opt, Camino Centenario & 506,Gonnet, RA-1897 La Plata, Buenos Aires, Argentina
[3] Univ Nacl La Plata, Fac Ciencias Exactas, 115 & 50, RA-1900 La Plata, Buenos Aires, Argentina
来源
APPLIED PHYSICS B-LASERS AND OPTICS | 2024年 / 130卷 / 11期
关键词
MUELLER-MATRIX POLARIMETRY; LIQUID-CRYSTAL; NONPHOTOREFRACTIVE MECHANISM; ERROR ANALYSIS; STOKES-VECTOR; COEFFICIENT; ACCURACY; CALIBRATION; DISPERSION; BI12TIO20;
D O I
10.1007/s00340-024-08327-5
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Using a non-holographic optical setup, we employed a Mueller-Stokes polarimeter to measure both the linear electro-optic and second-order electrogyration effects. The second-order electrogyration effect was observed in a Bi12SiO20\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Bi_{12}SiO_{20}$$\end{document} (BSO) crystal with a (110) cut. This response was found for the electric field applied both parallel and perpendicular to the [001] direction, where the values for the second-order electrogyration are 4.86x107pm2/V2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$4.86\times 10<^>{7} \, \text {pm}<^>{2}/\text {V}<^>{2}$$\end{document} and 1.87x107pm2/V2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$1.87\times 10<^>{7} \, \text {pm}<^>{2}/\text {V}<^>{2}$$\end{document}, respectively. Additionally, the linear electro-optic coefficient gamma 41\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\gamma _{41}$$\end{document} was measured to be 1.17pm/V\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$1.17 \, \text {pm/V}$$\end{document} for 660.5nm\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$660.5 \, \text {nm}$$\end{document}.
引用
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页数:11
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